A charge $Q$ is distributed over three concentric spherical shell of radii $a, b, c (a < b < c)$ such that their surface charge densities are equal to one another. The total potential at a point at distance $r$ from their common centre, where $r < a$, would be
$\frac{Q}{{12\pi \,{ \in _0}}}\frac{{ab + bc + ca}}{{abc}}$
$\frac{{Q\,\left( {{a^2} + {b^2} + {c^2}} \right)}}{{4\pi \,{ \in _0}\,\left( {{a^3} + {b^3} + {c^3}} \right)\,}}$
$\frac{Q}{{4\pi \,{ \in _0}\,\left( {a + b + c} \right)\,}}$
$\frac{{Q\,\left( {a + b + c} \right)}}{{4\pi \,{ \in _0}\,\left( {{a^2} + {b^2} + {c^2}} \right)\,\,}}$
Consider a finite insulated, uncharged conductor placed near a finite positively charged conductor. The uncharged body must have a potential
Let $V$ and $E$ are potential and electric field intensity at a point then
In a region, if electric field is defined as $\vec E = \left( {\hat i + 2\hat j + \hat k} \right)\,V/m$ , then the potential difference between two points $A (0, 0, 0)$ and $B (2, 3, 4)$ in that region, is ......$V$
Two charge $ + \,q$ and $ - \,q$ are situated at a certain distance. At the point exactly midway between them
Is electrostatic potential vector or scalar ?